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. 2019 Mar 22;4(3):5714–5721. doi: 10.1021/acsomega.9b00056

Figure 1.

Figure 1

(a) Top (upper panel) and side (bottom panel) views of crystal structure of bulk NiX2 (X = Cl, Br, I). (b) Super cell model with introduced fracture used to simulate the exfoliation procedure. (c) Cleavage energy Ecl as a function of the separation between two fractured parts. (d) Variation of relative energy with the 2D lattice constant for the monolayer of NiX2. The energy of equilibrium state is set to 0. (e) NiX2 monolayer. d0 is the vertical distance between two halide atomic planes.